Departamento de Física, Universidad Autónoma Metropolitana-Iztapalapa, Av. San Rafael Atlixco 186, Col. Vicentina, 09340 México DF.
J Chem Phys. 2011 Aug 28;135(8):084126. doi: 10.1063/1.3628675.
Liquid-vapor interfacial properties of square well chains are calculated. Surface tension, orthobaric densities, and vapor pressures are reported. Spinodal decomposition with a discontinuous molecular dynamics simulation program is used to obtain the results which are compared to previously published data for orthobaric densities and vapor pressures. In order to analyze the effect of the chain stiffness results for near tangent and overlapping linear chains as well as angled chains are obtained. Properties are calculated for linear chains of 2, 4, and 8 spheres for intramolecular distances of 0.97, 0.6, and 0.4 as well as for angled chains of 4 and 8 spheres and intramolecular distances of 0.4. The complete series of fully flexible near tangent square well chains is also studied (chains of 2, 4, 8, 12, and 16 particles with intramolecular distances of 0.97). The corresponding states principle applies to most of the systems considered. Critical properties values are reported as obtained from orthobaric densities, surface tensions, and vapor pressures. For the near tangent chains the critical temperatures increase with chain length but the rate of increment tends to zero for the longest chains considered. When the stiffness of the chain increases (intramolecular distance from 1 , 0.6, and 0.4) this saturation effect is either not present or reverses itself. The surface tension increases with the length of the chain while the width of the interface decreases.
计算了方阱链的液-气相界面性质。报告了表面张力、等压密度和蒸气压。使用不连续分子动力学模拟程序进行旋节分解以获得结果,并将其与等压密度和蒸气压的先前发表数据进行比较。为了分析链刚度的影响,还获得了近相切和重叠线性链以及成角度链的结果。计算了分子内距离为 0.97、0.6 和 0.4 的 2、4 和 8 个球体的线性链以及分子内距离为 0.4 的 4 和 8 个球体的成角度链的性质。还研究了完整系列的完全灵活的近相切方阱链(分子内距离为 0.97 的 2、4、8、12 和 16 个粒子的链)。大多数考虑的系统都适用对应状态原理。报告了从等压密度、表面张力和蒸气压获得的临界性质值。对于近相切链,临界温度随链长增加而增加,但对于考虑的最长链,增加速率趋于零。当链的刚度增加(分子内距离为 1、0.6 和 0.4)时,这种饱和效应要么不存在,要么相反。表面张力随链长的增加而增加,而界面的宽度减小。